Why is the heaviside function in the inverse Laplace transform of 1?

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Discussion Overview

The discussion revolves around the inverse Laplace transform of the constant function 1 and the presence of the Heaviside function in this context. Participants explore the definitions and implications of the Laplace transform, particularly focusing on the relationship between the Heaviside function and the constant function across different intervals.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants note that the Laplace transform of a function f(t) is defined as the integral from 0 to infinity of f(t)e^{-st}dt, and question why the Heaviside function appears in the inverse transform of 1/s.
  • Others argue that the Heaviside function is defined as 0 for x < 0, 1/2 for x = 0, and 1 for x > 0, and in the context of the Laplace integral, it behaves like the constant function f(x) = 1 for t ≥ 0.
  • A participant mentions a broader problem involving the inverse Laplace transform of a more complex expression and questions whether the Heaviside function can replace a constant term in their result.
  • Another participant expresses confusion regarding the multiplication of terms by the Heaviside function and the structure of the partial fraction decomposition presented.
  • One participant clarifies their use of a theorem related to the Heaviside function and its role in shifting the function in the inverse transform, correcting their earlier misunderstanding about the substitution variable.
  • Another participant emphasizes the importance of defining functions for negative values of t, noting that the Heaviside function accounts for these definitions in the context of Laplace transforms.

Areas of Agreement / Disagreement

Participants express differing views on the role of the Heaviside function in the inverse Laplace transform of 1/s. While some agree on its definition and implications, others contest the necessity of including it in certain contexts, leading to an unresolved discussion.

Contextual Notes

There are limitations regarding the assumptions made about the definitions of functions for negative values of t, and the discussion reflects varying interpretations of the Heaviside function's role in the Laplace transform framework.

Blanchdog
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Homework Statement:: Why is the heaviside function in the inverse laplace transform of 1?
Relevant Equations:: N/A

This is a small segment of a larger problem I've been working on, and in my book it gives the transform of 1 as 1/s and vice versa. But as I've looked online for help in figuring parts of this out, I keep seeing that the heaviside function is the inverse laplace transform of 1/s, when I would think (according to my book) that it should just be 1. Can anyone explain this?
 
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Blanchdog said:
Homework Statement:: Why is the heaviside function in the inverse laplace transform of 1?
Relevant Equations:: N/A

This is a small segment of a larger problem I've been working on, and in my book it gives the transform of 1 as 1/s and vice versa. But as I've looked online for help in figuring parts of this out, I keep seeing that the heaviside function is the inverse laplace transform of 1/s, when I would think (according to my book) that it should just be 1. Can anyone explain this?
The Laplace transform of a function f(t), defined on the real numbers, is ##\int_0^\infty f(t)e^{-st}dt##. The Heaviside function, H(x), is defined to be 0 for x < 0, 1/2 for x = 0, and 1 for x > 0. For the interval in the Laplace integral, the Heaviside function is identical to the constant function f(x) = 1.
 
Mark44 said:
The Laplace transform of a function f(t), defined on the real numbers, is ##\int_0^\infty f(t)e^{-st}dt##. The Heaviside function, H(x), is defined to be 0 for x < 0, 1/2 for x = 0, and 1 for x > 0. For the interval in the Laplace integral, the Heaviside function is identical to the constant function f(x) = 1.

Okay, so in the context of the broader problem: $$x=L^{-1} \frac{e^(-2s)}{s(s+2)^2} $$ In which I get the result $$x = \frac{H(t-2)}{4}(1 -e^{4-2t}+2te^{4-2t}-4e^{4-2t})$$ The first term could be replaced by ##H(t-2)## and both would be correct?
 
Blanchdog said:
Okay, so in the context of the broader problem: $$x=L^{-1} \frac{e^(-2s)}{s(s+2)^2} $$ In which I get the result $$x = \frac{H(t-2)}{4}(1 -e^{4-2t}+2te^{4-2t}-4e^{4-2t})$$ The first term could be replaced by ##H(t-2)## and both would be correct?
I'm not sure what you're doing above.
$$\mathcal L^{-1}[\frac{e^{-2s}}{s(s + 2)^2}] = \mathcal L^{-1}[ \frac{1/4e^{-2s}}{s} + \frac{-1/4e^{-2s}}{s+2} + \frac{-1/2e^{-2s}}{(s + 2)^2}]$$
I don't know why you have four terms inside the parentheses or why you have H(t-2) multiplying those four terms.
 
Mark44 said:
I'm not sure what you're doing above.
$$\mathcal L^{-1}[\frac{e^{-2s}}{s(s + 2)^2}] = \mathcal L^{-1}[ \frac{1/4e^{-2s}}{s} + \frac{-1/4e^{-2s}}{s+2} + \frac{-1/2e^{-2s}}{(s + 2)^2}]$$
I don't know why you have four terms inside the parentheses or why you have H(t-2) multiplying those four terms.
I broke up the last term because it was multiplied by ##(t-1)##. I also got the last term as being positive rather than negative in my partial fraction expansion.

EDIT: Found my algebra error, your partial fraction expansion is right.
 
Last edited:
I didn't work out the inverse Laplace transforms of what I showed. All I did was to get the partial fraction decomposition.
$$\frac 1 {s(s + 2)^2} = \frac {1/4}{s} + \frac{-1/4}{s+ 2} + \frac{-1/2}{(s + 2)^2}$$
I've checked my work, so I'm pretty confident of the coefficients.

I don't understand what you're saying about being multiplied by t - 1. I also don't understand why you have H(t - 2) multiplying all of your terms.
 
I've used the theorem ##L (H(t-c)*f(t-c)) = e^{-cs} F(s)##, where the partial fraction expansion above is ##F(s)##, and ##c = 2##. Since the problem is of the form of this theorem, the inverse transform results in a heaviside function multiplied by the inverse transform of ##F(s)## with t substituted by ##(t-c)##, in this case ##(t-2)## (not 1, I misread my work before).
 
Blanchdog said:
I've used the theorem L(H(t−c)∗f(t−c))=e−csF(s), where the partial fraction expansion above is F(s), and c=2. Since the problem is of the form of this theorem, the inverse transform results in a heaviside function multiplied by the inverse transform of F(s) with t substituted by (t−c), in this case (t−2) (not 1, I misread my work before).
Be careful when you write ##\mathcal L[H(t - c) * f(t - c)]##. I took this at first to mean the transform of the convolution of H(t - c) and f(t - c). Not that the symbol '*' is used for convolution.
Some definitions:
$$f(t) * g(t) = \int_0^1 f(t - x)g(x)dx$$
$$\mathcal L[f(t) * g(t)] = F(s)G(s)$$

Regarding your problem, with the wrinkles removed, do you still have any questions?
 
Last edited:
When you take a Laplace Transform of a function ##f##, you typically ignore what ##f(t)## is for negative values of ##t##, so when the table says ##f(t)=1##, what it really means is ##f(t)=1## for ##t\ge 0##. But when you shift this function to the right, the value of ##f(t)## for negative values of ##t## becomes important, and it's assumed that ##f(t)=0## for ##t<0##. So the full definition of ##f## is really
$$f(t) = \begin{cases} 1 & t \ge 0 \\ 0 & t<0 \end{cases},$$ which you should recognize is one of the possible definitions for the Heaviside step function.

On a related note, when you invert, say, ##F(s) = \frac 1{s+a}## and get ##f(t) = e^{-at}##, it's understood that this result is valid only for ##t\ge 0##. Technically, you should write ##f(t) = e^{-at} H(t)##, but pedantically including the step function can get tedious, so it's often omitted and assumed that the reader knows it's there.
 

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